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  1. 3.4 First law of thermodynamics – internal energy The first law of thermodynamics expresses that energy is conserved, when all forms of energy, including heat, are taken into account.

  2. Internal energy is a state function and an extensive prop-erty. One can have a corresponding intensive thermodynamic property called specific internal energy, u, which is internal energy per mass of the substance. Table 4.1 shows the different components of internal energy of a system, while Table 4.2 shows the changes in internal energy.

  3. Enthalpy: Enthalpy is defined as the total heat content or total useful energy of a substance. The symbol for enthalpy is “h.” Enthalpy is also considered to be the sum of internal energy “u” and flow energy (or flow work) p.V. This definition of enthalpy can be expressed, mathematically, as follows: h = u + p.V Eq. 1.1 Where,

  4. If you have a system with constant volume (and variable pressure), the best suited state function is the free energy F (also called Helmholtz energy). It is defined as. F = U – T · S. Before turning to the entropy, a word to the choice of state functions.

  5. Thermodynamics Unit ­ Internal Energy, Work and Heat 1. The internal energy of a system increased by 982 J when it absorbed 492 J of heat. Was work done by or on the system? How much work was done? What is ΔV if pressure is constant at 1 atm? €

  6. In Thermodynamics, the total energy E of our system (as described by an empirical force field) is called internal energy U. U is a state function, which means, that the energy of a system depends only on the values of its parameters, e.g. T and V, and not on the path in the parameters space, which led to the actual state.

  7. ctly involved.4 Internal energy is a function of state. Heat and work are not functions of state.5 The first law of thermodynamics states that, if a system undergoes a change from one equilibrium state to another, the difference between the heat Q supplied to the system and the work W done by the system will depend.

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